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First Law Closed System Formulas ISOMETRIC (Isochoric) PROCESS a.) Relationship between P and T. T1/T2 = P1/P2 b.) Non-flow work. Wn = c.) The change of internal energy ΔU = mcv(T2 – T1) d.) The heat transferred Q = mcv(T2 – T1) e.) The change of enthalpy ΔH = mcp(T2 - T1) f.) Irreversible non-flow constant volume process Q = ΔU + Wn where: For reversible non-flow, Wn = 0 For irreversible nonflow, Wn ‡ 0 Wn = non-flow work ISOBARIC PROCESS a) Relationship between V and T T1/T2 = V1/V2 b) Nonflow work Wn = = P(V2 – V1) = mR(T2 – T1) c) Change of internal energy ΔU = mcv (T2 – T1) d) Heat transferred Q = mcp (T2 – T1) e) Change of enthalpy ΔH = mcp (T2 – T1) ISOTHERMAL PROCESS (a.) Relationship between P and V P1V1 = P2V2 (b.) Nonflow work Wn = P1V1lnV2/V1 = mRT1lnV2/V1 (c.) The change of internal energy ΔU = O (d.) The heat transferred Q = Wn = P1V1lnV2/V1 = mRT1lnP1/P2 (e.) The change of enthalpy ΔH = 0 ISENTROPIC PROCESS 1. Relationship among P, V and T. (a) Relationship between P and V P1V1 k = P2V2 k = C (b) Relation between T and V From P1 V1 k = P2 V2 k and P1V1/T1 = P2V2/T2, we have T2/T1 = [V1/V2] k-1 (c ) Relation between T and P T2/T1 = [p2/p1] (k-1)/k 2. Nonflow work. From PV k = C, P = CV -k Wn = PdV = C -k dV = C V -k dV Integrating and simplifying Wn = P2V2 – P1V1 / (1- k) = mR(T2 – T1) / (1 – k) 3. The change of internal energy. ΔU = mCv (T2 – T1) 4. The heat transferred. Q = 0 5. The change of enthalpy. ΔH = mCp (T2 – T1) 6. The change of entropy. ΔS = 0 POLYTROPIC PROCESS 1. Relationship among p, V, and T (a) Relation between P and V P1V1 n = P2V2 n (b) Relation between T and V T2/T1 = [V1/V2] n-1 (c) Relation between T and p T2/T1 = [p2/p1] (n-1)/n 2. Nonflow work Wn = ∫pdV = P2V2 – P1V1 / 1-n = mR(T2-T1) / 1-n 3. The change of internal energy. ΔU = mCv(T2 – T1) 4. The heat transferred. Q = ΔU + Wn = mcv (T2 – T1) + mR (T2 – T1)/(1 - n) = m [(cv – ncv + R)/(1 – n)] (T2 – T1) = m [(cp – ncv)/(1 – n)] (T2 – T1) = mcv [(k – n)/(1 – n)] (T2 – T1) Q = mCn(T2 – T1) Cn = Cv [(k – n)/(1 – n)], the polytropic specific heat 5. The change of enthalpy ΔH = mCp (T2 – T1)

FORMULA_First Law Closed, Open and Transient System Formulas

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  • First Law Closed System Formulas

    ISOMETRIC (Isochoric) PROCESS

    a.) Relationship between P and T.

    T1/T2 = P1/P2

    b.) Non-flow work.

    Wn =

    c.) The change of internal energy

    U = mcv(T2 T1)

    d.) The heat transferred

    Q = mcv(T2 T1)

    e.) The change of enthalpy

    H = mcp(T2 - T1)

    f.) Irreversible non-flow constant volume process

    Q = U + Wn

    where: For reversible non-flow, Wn = 0

    For irreversible nonflow, Wn 0

    Wn = non-flow work

    ISOBARIC PROCESS

    a) Relationship between V and T

    T1/T2 = V1/V2

    b) Nonflow work

    Wn = = P(V2 V1) = mR(T2 T1)

    c) Change of internal energy

    U = mcv (T2 T1)

    d) Heat transferred

    Q = mcp (T2 T1)

    e) Change of enthalpy

    H = mcp (T2 T1)

    ISOTHERMAL PROCESS

    (a.) Relationship between P and V

    P1V1 = P2V2

    (b.) Nonflow work

    Wn = P1V1lnV2/V1 = mRT1lnV2/V1

    (c.) The change of internal energy

    U = O

    (d.) The heat transferred

    Q = Wn = P1V1lnV2/V1 = mRT1lnP1/P2

    (e.) The change of enthalpy

    H = 0

    ISENTROPIC PROCESS

    1. Relationship among P, V and T.

    (a) Relationship between P and V

    P1V1k = P2V2k = C

    (b) Relation between T and V

    From P1 V1k = P2 V2k and P1V1/T1 = P2V2/T2, we have

    T2/T1 = [V1/V2]k-1

    (c ) Relation between T and P

    T2/T1 = [p2/p1](k-1)/k

    2. Nonflow work.

    From PVk = C, P = CV-k

    Wn = PdV = C-kdV = C V-kdV

    Integrating and simplifying

    Wn = P2V2 P1V1 / (1- k) = mR(T2 T1) / (1 k)

    3. The change of internal energy.

    U = mCv (T2 T1)

    4. The heat transferred.

    Q = 0

    5. The change of enthalpy.

    H = mCp (T2 T1)

    6. The change of entropy.

    S = 0

    POLYTROPIC PROCESS

    1. Relationship among p, V, and T

    (a) Relation between P and V

    P1V1n = P2V2n

    (b) Relation between T and V

    T2/T1 = [V1/V2]n-1

    (c) Relation between T and p

    T2/T1 = [p2/p1](n-1)/n

    2. Nonflow work

    Wn = pdV = P2V2 P1V1 / 1-n = mR(T2-T1) / 1-n

    3. The change of internal energy.

    U = mCv(T2 T1)

    4. The heat transferred. Q = U + Wn

    = mcv (T2 T1) + mR (T2 T1)/(1 - n)

    = m [(cv ncv + R)/(1 n)] (T2 T1)

    = m [(cp ncv)/(1 n)] (T2 T1)

    = mcv [(k n)/(1 n)] (T2 T1)

    Q = mCn(T2 T1)

    Cn = Cv [(k n)/(1 n)], the polytropic specific heat

    5. The change of enthalpy

    H = mCp (T2 T1)

  • First Law Open System Formulas

    Mass:

    Energy:

    Nozzle/Diffuser:

    2 2

    1 21 20

    2

    V Vh h

    Turbine and Compressor:

    Heat Exchangers:

    2 2

    2 2

    i ei i i e e e

    i e

    V Vm h gz m h gz

    Throttling Device:

    i eh h

    Transient System

    Mass:

    Energy:

    cvi e

    i e

    dmm m

    dt

    2 2

    2 2

    cv i ecv cv i i i e e e

    i e

    dE V VQ W m h gz m h gz

    dt

    2 2

    1 21 2 1 2

    2

    W V Vh h g z z

    m

    0cv cv i ei e

    m t m m m

    0 0

    0t t

    cv cv cv cv i i e e

    i e

    U t U Q W m hdt m h dt